CN1302102A - High power tunable CO2 laser - Google Patents
High power tunable CO2 laser Download PDFInfo
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- CN1302102A CN1302102A CN 99127121 CN99127121A CN1302102A CN 1302102 A CN1302102 A CN 1302102A CN 99127121 CN99127121 CN 99127121 CN 99127121 A CN99127121 A CN 99127121A CN 1302102 A CN1302102 A CN 1302102A
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- perot modulator
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Abstract
The CO2 laser includes one spherial reflector, one CO2 laser discharging gain region, and one Fabry-Perot modulator and features that the Fabry-Perot modulator is as one terminal reflector of the laser resonant cavity and for laser power to be transmitted to couple output. With simple structure and stable performance, the CO2 laser may be applied in laser chemistry, atmosphere transmission, material machining and other fields.
Description
The invention belongs to laser, particularly a kind of high power tunable CO 2 (CO that adopts Fabry-Perot modulator as the selection of laser transition band
2) laser.
The Fabry-Perot interference tool is widely used in tunable laser, particularly tunable CO
2In the laser.Usually the technology that adopts is to insert the Fabry-Perot interference tool of inclination in laserresonator.Fig. 1 is the tunable CO that adopts inclination Fabry-Perot interference tool in the chamber
2The laser schematic diagram.As shown in Figure 1, laserresonator is made up of the level crossing 14 of sphere completely reflecting mirror 11 and partial reflection.Laser beam 16 is from level crossing 14 transmissions coupling output.Also inserted the Fabry-Perot interference tool 13 that a pair of level crossing that is parallel to each other is formed in the laserresonator except that laser gain district 12, the spacing between the level crossing is d, and inner surface has identical reflectivity, outer surface coating anti reflection film.Rotation interferes the inclination angle [theta] of tool can realize the tuning of laser.The shortcoming of this technology is coupling loss (seeing the reflection coupled light beam 15 of accompanying drawing 1) can occur reflecting at two reflectings surface of interfering tool.Because the laser that the present invention relates to is to operate under the high-power condition, so the Fabry-Perot interference tool should be selected low acutance for use.Because the too high light intensity of interfering in the tool that will make of acutance causes interfering the damage of tool minute surface too by force.Under the situation of low acutance, in tuning process, rotational angle theta changes a certain transition line in all exportable a certain transition band in certain scope, but interfere tool only on a certain specific angle θ reflectivity just be that zero (supposition interferes the absorption of tool to ignore, then transmitance is 1), laser could all be exported from outgoing mirror.When slightly departing from θ, though laser also be tuned on same transition line, non-vanishing from the reflection of interfering tool, therefore the part laser energy is arranged from two reflectings surface coupling outputs.The appearance of reflection coupling makes laser beam splitting occur, can reduce the efficient of transmission coupling, and makes the very big fluctuating of laser output power generation in tuning process.In superpower laser, the light beam that also is necessary for the reflection coupling increases output window, and this also makes troubles for laser design.
The objective of the invention is to propose a kind of high power tunable CO
2Laser, the optical maser wavelength of its output can be apace be tuned to CO
2A transition band in four transition bands of molecule (P of 00 ° of 1-10 ° of 0 band and 00 ° of 1-02 ° of 0 band props up with R and props up).
A kind of high power tunable CO 2 laser of the present invention, comprise spherical reflector, carbon dioxide laser discharge gain region, Fabry-Perot modulator, it is characterized in that, wherein Fabry-Perot modulator is a terminal reflector of laserresonator, and laser power is from Fabry-Perot modulator transmission coupling output.
Wherein laser output wavelength (frequency) can be tuned to a transition band in four transition bands (00 ° of 1-10 ° of 0 band and 00 ° of 1-02 ° of 0 P that is with prop up with R and prop up) of carbon dioxide molecule.
Wherein laser output average power or continuous power are 10 watts-2 * 10
4Watt.
Wherein laser output pulse peak power is 10
2Watts-10
9Watt.
Wherein the reflectivity of the speculum of Fabry-Perot modulator is 0.1-0.5.
Wherein the mirror spacing of the speculum of Fabry-Perot modulator is the 0-100 micron.
Wherein the mirror spacing of the speculum of Fabry-Perot modulator adopts the fine setting motor to regulate.
Wherein the mirror spacing of the speculum of Fabry-Perot modulator adopts piezoelectric ceramic to regulate.
Wherein the speculum of Fabry-Perot modulator is the zinc selenide speculum of single face coating anti reflection film.
Wherein the speculum of Fabry-Perot modulator is the GaAs speculum of single face coating anti reflection film.
Wherein the speculum of Fabry-Perot modulator is the germanium speculum of single face coating anti reflection film.
For further specifying feature of the present invention and structure, below in conjunction with accompanying drawing the present invention is made a detailed description, wherein:
Fig. 1 is the tunable CO that adopts inclination Fabry-Perot interference tool in the chamber
2The laser schematic diagram;
Fig. 2 is a principle assumption diagram of the present invention;
Fig. 3 is normalized CO
2Laser transition small signal gain distribution map;
Fig. 4 is laser tuning theoretical principle figure of the present invention, and left is the relation of laser transition net gain coefficient and jump frequency, and right-hand is the reflectivity of Fabry-Perot modulator and the relation of jump frequency.Wherein the relevant selection of parameter of laser is TEA (transverse excitation atmosphere) CO
2Laser gain section length l=100cm, the small signal gain coefficient α of the strongest line in the gain spectral (normally 10P (20) line of 10P band)
0=0.02cm
-1, the reflectivity R of Fabry-Perot modulator speculum
0=0.17, mirror spacing is got 20.4 μ m respectively for (A), (B), (C), (D) of Fig. 4,21.7 μ m, 22.3 μ m, 24.1 μ m.
Please consult normalized CO shown in Figure 3 earlier
2The laser transition small signal gain is with the distribution of frequency.CO
2The laser transition spectral line can have about 100 in 9 to 11 mum wavelength scopes, adheres to 10P, 10R, four transition bands of 9P, 9R (P of 00 ° of 1-10 ° of 0 band and 00 ° of 1-02 ° of 0 band props up with R and props up) separately.The peak value spectral line of four transition bands is respectively 10P (20), 10R (18), 9P (20) and 9R (18) as can be seen from Figure.But in resonant cavity without any the free-running TEA CO of dispersion element
2In the laser, because the result of gain competition, laser output power always concentrates on the highest spectral line of gain.The gain of 10P (20) transition line is the highest, therefore free-running TEACO
2The laser transition line of laser output is 10P (20), and laser frequency is 945cm
-1, wavelength is 10.6 μ m.
For obtaining the laser transition line output of other transition band, the present invention adopts the output reflector of Fabry-Perot modulator as resonant cavity.As shown in Figure 2, laserresonator is made up of spherical reflector 21 and Fabry-Perot modulator 23, and wherein Fabry-Perot modulator is a terminal reflector of laserresonator, and laser power is from Fabry-Perot modulator transmission coupling output.Laser gain district 22 length are l, and laser beam is from Fabry-Perot modulator transmission coupling output.The reflectivity of desirable Fabry-Perot modulator is provided by following formula:
R in the following formula
0Be the reflectivity of Fabry-Perot modulator single-surface mirror, v is a laser frequency, and d is the Fabry-Perot modulator mirror spacing, and c is the light velocity.Scattering and the absorption loss of having ignored Fabry-Perot modulator in the formula.The reflectivity of the example explanation Fabry-Perot modulator that Fig. 4 provides is with the variation of frequency v and mirror spacing d.Parameters R
0Get 0.17, corresponding to the single face reflectivity of uncoated zinc selenide mirror.
For the jump frequency of determining that laser may be exported, also need to obtain the net gain of round trip in the laserresonator with the distribution G of frequency (v):
G(v)=2lα
0g(v)+1nR(v)
L is discharge gain region length, α in the following formula
0Be the small signal gain coefficient of 10P (20) line, g (v) is the normalized gain profiles factor.R (v) is the reflectivity of Fabry-Perot modulator.Ignored the loss of the other types in the resonant cavity in the formula, as the absorption of the diffraction loss of resonator mode, optical element and scattering etc.
In the example that Fig. 4 provides, α
0=0.02cm
-1, l=100cm, R
0=0.17.Appropriate as can be seen from Figure selection different mirror spacing d, the peak value that net gain distributes appears at respectively in four different transition bands, so laser can be tuning between these four transition bands.Adopt piezoelectric ceramic to regulate the spacing of modulator, can realize electric tuning fast.This scheme is applicable to high-average power Tunable TEA CO
2The continuous CO of laser or high power tunable
2Laser.
The present invention has simple in structure, and is stable and reliable for performance, can be widely used in laser chemistry, big The advantage in the fields such as gas transmission, materials processing.
Claims (11)
1, a kind of high power tunable CO 2 laser comprises spherical reflector, carbon dioxide laser discharge gain region, Fabry-Perot modulator, it is characterized in that,
Wherein Fabry-Perot modulator is a terminal reflector of laserresonator, and laser power is from Fabry-Perot modulator transmission coupling output.
2, a kind of high power tunable CO 2 laser according to claim 1, it is characterized in that, wherein laser output wavelength (frequency) can be tuned to a transition band in four transition bands (00 ° of 1-10 ° of 0 band and 00 ° of 1-02 ° of 0 P that is with prop up with R and prop up) of carbon dioxide molecule.
3, a kind of high power tunable CO 2 laser according to claim 1 is characterized in that, wherein laser output average power or continuous power are 10 watts-2 * 10
4Watt.
4, a kind of high power tunable CO 2 laser according to claim 1 is characterized in that, wherein laser output pulse peak power is 10
2Watts-10
9Watt.
5, a kind of high power tunable CO 2 laser according to claim 1 is characterized in that, wherein the reflectivity of the speculum of Fabry-Perot modulator is 0.1-0.5.
6, a kind of high power tunable CO 2 laser according to claim 1 is characterized in that, wherein the mirror spacing of the speculum of Fabry-Perot modulator is the 0-100 micron.
7, a kind of high power tunable CO 2 laser according to claim 1 is characterized in that, wherein the mirror spacing of the speculum of Fabry-Perot modulator adopts the fine setting motor to regulate.
8, a kind of high power tunable CO 2 laser according to claim 1 is characterized in that, wherein the mirror spacing of the speculum of Fabry-Perot modulator adopts piezoelectric ceramic to regulate.
9, a kind of high power tunable CO 2 laser according to claim 1 is characterized in that, wherein the speculum of Fabry-Perot modulator is the zinc selenide speculum of single face coating anti reflection film.
10, a kind of high power tunable CO 2 laser according to claim 1 is characterized in that, wherein the speculum of Fabry-Perot modulator is the GaAs speculum of single face coating anti reflection film.
11, a kind of high power tunable CO 2 laser according to claim 1 is characterized in that, wherein the speculum of Fabry-Perot modulator is the germanium speculum of single face coating anti reflection film.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| CNB991271211A CN1136635C (en) | 1999-12-28 | 1999-12-28 | High power tunable CO2 laser |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| CNB991271211A CN1136635C (en) | 1999-12-28 | 1999-12-28 | High power tunable CO2 laser |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| CN1302102A true CN1302102A (en) | 2001-07-04 |
| CN1136635C CN1136635C (en) | 2004-01-28 |
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ID=5284724
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| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| CNB991271211A Expired - Fee Related CN1136635C (en) | 1999-12-28 | 1999-12-28 | High power tunable CO2 laser |
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| Country | Link |
|---|---|
| CN (1) | CN1136635C (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN102208749A (en) * | 2011-04-15 | 2011-10-05 | 中国人民解放军国防科学技术大学 | Intermediate and far infrared two-waveband laser |
-
1999
- 1999-12-28 CN CNB991271211A patent/CN1136635C/en not_active Expired - Fee Related
Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN102208749A (en) * | 2011-04-15 | 2011-10-05 | 中国人民解放军国防科学技术大学 | Intermediate and far infrared two-waveband laser |
| CN102208749B (en) * | 2011-04-15 | 2012-06-27 | 中国人民解放军国防科学技术大学 | Intermediate and far infrared two-waveband laser |
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| Publication number | Publication date |
|---|---|
| CN1136635C (en) | 2004-01-28 |
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| CB03 | Change of inventor or designer information |
Inventor after: Wan Zhongyi Inventor after: Wan Peng Inventor after: Tan Rongqing Inventor after: Wu Jin Inventor before: Wan Zhongyi |
|
| COR | Change of bibliographic data |
Free format text: CORRECT: INVENTOR; FROM: WAN ZHONGYI TO: WAN ZHONGYI; WAN PENG; TAN RONGQING; WU JIN |
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| C19 | Lapse of patent right due to non-payment of the annual fee | ||
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